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SET-PARTITION TABLEAUX Tom Halverson Macalester College FPSAC 2019 - - PowerPoint PPT Presentation
SET-PARTITION TABLEAUX Tom Halverson Macalester College FPSAC 2019 - - PowerPoint PPT Presentation
SET-PARTITION TABLEAUX Tom Halverson Macalester College FPSAC 2019 Ljubljana July 2, 2019 1/25 Set-Partition Tableaux Integer Partition: Organization: I. Origins: Representation 8 , 13 14 Theory of the Symmetric 2 , 3 1 , 6 , 10 16
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Set-Partition Tableaux
Integer Partition:
8, 13 14 2, 3 1, 6, 10 16 4 12 5, 7, 9 15, 17 11
Set Partition: 8 > > < > > : {2, 3}, {4}, {5, 7, 9}, {1, 6, 10}, {11}, {12}, {8, 13}, {14}, {16}, {15, 17} 9 > > = > > ; Organization:
- I. Origins: Representation
Theory of the Symmetric Group
- II. Schur-Weyl Duality: The
Partition Algebra and Other Diagram Algebras
- III. Insertion Bijections
May 2016: [Benkart-H-Harmon] Dimensions of irreducible modules ... [Orellana-Zabrocki] Symmetric group characters as symmetric functions
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- I. Symmetric Group Tensor Power Representations
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Origins: The Symmetric Group Sn
I Mn = n-dimensional permutation module ⇠ = Sn Sn
I Basis: v1, v2, . . . , vn with group action: (vi) = vσ(i)
I Sλ
n = irreducible CSn-module, ` n
I M⌦k
n
= k-fold tensor product module
I Diagonal action on basis of simple tensors: (vi1 ⌦ vi2 ⌦ · · · ⌦ vik) = vσ(i1) ⌦ vσ(i2) ⌦ · · · ⌦ vσ(ik)
Question Determine the multiplicity mλ
k,n in the decomposition:
M⌦k
n
= M
λ`n
mλ
k,n Sλ n
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Method 1: Restriction-Induction
Tensor Identity: tensoring with the permutation module is the same as restriction and induction Sλ
n ⌦ Mn ⇠
= IndSn
Sn−1ResSn Sn−1(Sλ n)
⇠ = IndSn
Sn−1
M
ν=λ⇤
Sν
n1
⇠ = M
µ=ν+⇤
M
ν=λ⇤
Sµ
n
Sλ
n ⌦ Mn ⇠
= M
µ=(λ⇤)+⇤
Sµ
n
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Bratteli Diagram: B(S5, S4) for M⌦k
5 M⊗0
5
1
M⊗.5
5
1
M⊗1
5
1 1
M⊗1.5
5
2 1
M⊗2
5
2 3 1 1
M⊗2.5
5
5 5 1 1
M⊗3
5
5 10 6 6 2 1
M⊗3.5
5
15 22 8 9 1
. . . . . . . . . . . . . . . . . .
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Vacillating Tableaux
A vacillating tableaux of shape ` n is a sequence of partitions for which i+ 1
2 = i ⇤
and i+1 = i+ 1
2 + ⇤.
Example: A vacillating tableaux of length 6 and shape :
1 2 3 4 5 6
The multiplicity of Sλ
n in M⌦k n
is given by mλ
k,n = # vacillating tableaux of length k and shape .
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Method 2: Decompose M⌦k
n
into Permutation Modules
I Diagonal Action: ( va ⌦ va ⌦ vb ⌦ va ⌦ vb ⌦ vc ⌦ vd ⌦ vc ) = vσ(a) ⌦ vσ(a) ⌦vσ(b) ⌦ vσ(a) ⌦vσ(b) ⌦ vσ(c) ⌦vσ(d) ⌦ vσ(c)
1 2 3 4 5 6 7 8
I Partition tensor positions: P = {1, 2, 4 | 3, 5 | 6, 8 | 7}: vij = vi` iff j ⇠ ` in P I As a, b, c, d vary over distinct elements of {1, . . . , n}, these simple tensors span a submodule isomorphic to the permutation module M(n4,1,1,1,1) = IndSn
Sn−4⇥S1⇥S1⇥S1⇥S1(1).
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Decompose M⌦k
n
into Permutation Modules
M⌦k
n
⇠ =
n
M
t=0
⇢k t
- M(nt,1t) ⇠
=
n
M
t=0
⇢k t M
λ`n
Kλ,(nt,1t)Sλ
n
⇠ =
n
M
t=0
M
λ`n
⇢k t
- fλ/(nt)Sλ
n
I ⇢k t
- = # set partitions of {1, . . . , k} into t subsets (Stirling 2nd )
I Kλ,(nt,1t) = Kostka number = #semistandard tableaux of shape filled with 0, . . . , 0 | {z }
nt
, 1, 2, . . . , t. I Example:
0 0 0 1 2 3 4 5 6 7 8 9
has = (5, 4, 2, 1), n = 12, t = 9.
I Kλ,(nt,1t) = fλ/(nt) = # standard tableaux shape /(n t)
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Decompose M⌦k
n
into Permutation Modules
M⌦k
n
⇠ = M
λ`n n
M
t=0
⇢k t
- fλ/(nt)Sλ
n
mλ
k,n = n
X
t=0
⇢k t
- fλ/(nt) = #
⇢ (P, T)
- P = partition of {1, . . . , k} into t parts
T= standard tableau of shape /(n t)
- Example. A standard set-partition tableau of shape = (5, 4, 2, 1)
P = {1, 6|4, 7, 9, 10|2, 11, 12|8, 14|15, 16|5, 13, 18|3, 17, 19|20} t = 8. n = 12 1, 6 4, 7, 9, 10 2, 11, 12 8, 14 15, 16 5, 13, 18 3, 17, 19 20 T =
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Set-Partition Tableaux ! Vacillating Tableaux
mλ
k,n = #
8 < : Standard set-partition tableaux of shape /(n k) 9 = ; = # 8 < : Vacillating tableaux
- f length k
and shape 9 = ; 8 < : 6 4 27 135 9 = ; ! (
1 2 3 4 5 6 7 )
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6 4 27 135
!
1 2 3 4 5 6 7
[BH’19] H-Benkart, [COSSZ’19] Colmenarejo, Orellana, Saliola, Schilling, Zabrocki
6 4 27 135 6 2 4 135 2 4 135 13 2 4 2 13 6 4 135 → 27 2 4 135 → 6 2 4 → 135 13 2 → 4 1 2 1 2 →13 1 → 2 → 1
- 1. Remove box containing
m = max(T)
- 2. Delete m from the box
- 3. Schensted insert box
in T>1
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- II. Schur-Weyl Duality and the Partition Algebra
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Centralizer Algebra of Sn on M⌦k
n
Centralizer Algebra: Zk,n := EndSn(M⌦k
n ) =
n 2 End(M⌦k
n )
- (x) = (x), 2 Sn
- Schur-Weyl Duality:
M⌦k
n
⇠ = M
λ`n
mλ
k,nSλ n
| {z }
as an Sn-module
⇠ = M
λ`n
fλZλ
k,n
| {z }
as a Zk,n-module
I mλ
k,n = multk(Sλ n) = dim(Zλ k,n) =
#(Standard Set-Partition Tableaux) I fλ = dim(Sλ
n) = mult(Zλ k,n) = # (Standard Tableaux)
Artin-Wedderburn theory: dim(Zk,n) = X
λ`n
(mλ
k,n)2
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Bratteli Diagram: B(S6, S5) = B(Zk,6)
k = 0
1
k = .5
1
k = 1
1 1
k = 1.5
2 1
k = 2
2 3 1 1
k = 2.5
5 5 1 1
k = 3
5 10 6 6 2 1 1
k = 3.5
15 22 9 9 2 1
Sum of Squares (Bell No’s) 1 1 2 5 22 + 32 + 11 + 12 =15 52 203 876
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Partition Algebra Pk(n)
[P.P. Martin, V.F.R. Jones, ⇡1993]
Basis of set partitions of {1, . . . , k, 10, . . . , k0}. 1 10 2 20 3 30 4 40 5 50 6 60 7 70 8 80 = ⇢ {1, 3, 40}, {2, 10}, {4, 5, 7}, {6, 80}, {8, 60}, {20, 30}, {50, 70}
- Multiplication given by diagram concatenation:
= n Generated by 3 types of diagrams: , ,
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Action of Pk(n) on Tensor Space M⌦k
n
Transposition: u1 u2 u3 u6 v7 v8 u5 u4 u1 u2 u3 u4 u5 u6 u7 u8 u1 u2 u3 u4 u6 v7 v8 v u1 u2 u3 u4 u5 u6 u7 u8 v =
n
X
i=1
vi
projection onto trivial module
δu4,u5 u1 u2 u3 u6 v7 v8 u4 u4 u1 u2 u3 u4 u5 u6 u7 u8 I Commutes with Sn: Pk(n) ! EndSn(M⌦k
n )
I is surjective I it is injective if n 2k the stable case I kernel? [Benkart-H’19]
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Irreducible Modules for the Partition Algebra
Schur-Weyl Duality: M⌦k
n
⇠ = M
λ`n
mλ
k,nSλ n
| {z }
as an Sn-module
⇠ = M
λ`n
fλPλ
k
| {z }
as a Pk(n)-module
I mλ
k,n = dim(Pλ k) = #(Standard Set-Partition Tableaux)
I fλ = dim(Sλ
n) = # (Standard Tableaux)
The irreducible partition algebra module: Pλ
k = C-span
⇢ vT
- T 2
⇢standard set-partition tableaux of shape Question Is there a combinatorial action analogous to Young’s repre- sentations of Sn on standard tableaux?
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Action on Basis Indexed by Set-Partition Tableaux
[H-Jacobson, 2018] · · · 3, 5, 6 11 1, 2 4 12 8, 9, 10 7, 13 1 2 3 4 5 6 7 8 9 10 11 12 13 4 10 13 = · · · 1, 2, 3 8, 11 9 5, 6, 7 12 4 10, 13 · · · 3, 5, 6 11 1, 2 4 12 8, 9, 10 7, 13 1 2 3 4 5 6 7 8 9 10 11 12 13
= · · · 5 8, 9 10, 12, 13 1, 2, 4 3, 6 1, 2, 4 7, 11 = 0
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Action of Generators
, ,
· · · 3, 5 1, 2 4 6 8 7, 9 1 2 3 4 5 6 7 8 9 = · · · 1, 3 2, 4 5 7 6 8, 9
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Action of Generators
, ,
· · · 3, 5 1, 2 4 6 8 7, 9 1 2 3 4 5 6 7 8 9
= · · · 2 3, 5 1 4 6 8 7, 9
· · · 3, 5 1, 2 4 6 8 7, 9 1 2 3 4 5 6 7 8 9
= · · · 4 3, 5 1, 2 6 8 7, 9 = 0
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Action of Generators
, ,
· · · 3, 5 1, 2 4 6 8 7, 9 1 2 3 4 5 6 7 8 9
= · · · 1,2,3,5 4 6 8 7, 9
· · · 3, 5 1, 2 4 6 8 7, 9 1 2 3 4 5 6 7 8 9 = · · · 3, 5 1, 2 4 8 6,7,9 = 0
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Restricts Naturally to Subalgebras of the Partition Algebra
Brauer Algebra (matchings)
· · · 1, 5 6, 9 2 4 7 3 8
Rook Brauer Algebra (partial matchings)
· · · 2 1, 4 5 6, 8 3 9 7
Temperley-Lieb (planar matchings)
· · · 2, 3 1, 5 8, 9 4 6 7
Motzkin Algebra (planar partial matchings)
· · · 3, 4 5 8 7, 9 1 2 6
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Restricts Naturally to Subalgebras of the Partition Algebra
Symmetric Group (permutations)
· · · 1 2 5 8 3 4 9 6 7
Rook Monoid (partial permutations)
· · · 3 4 5 7 1 2 8 6 9
Identity (planar permutations)
1 2 3 4 5 6 7 8 9 · · ·
Planar Rook Monoid (planar partial permutations)
· · · 1 2 3 5 6 9 4 7 8
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- III. Insertion Bijections
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- III. Insertion Bijections:
dim(P
k(n)) =
X
`n
(m
k,n)2
1 2 3 4 5 6 1 2 3 4 5 6
@
1,3 2 4 5,6
,
5 2,3 6 1,4
1 A P = ⇣
1 2 3 4 5 6
⌘ Q = ⇣
1 2 3 4 5 6
⌘
[COSSZ’19] [HL’04] [CDDSY’06] [BH’19]∗ [COSSZ’19]
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[HL’04] [COSSZ’19]
1 2 3 4 5 6 1 2 3 4 5 6
5 2,3,7,8 6,9 1,4,11 10,12 5 2,3,7,8 6,9 1,4,11 10 5 2,3,7,8 6,9 1,4 10 5 2,3,7,8 6,9 1,4 5 2,3,7,8 1,4 6 5 1,4 6 2,3,7 5 2,3 1,4 6 5 2,3,7,8 6,9 1,4,11 10,12 5 2,3,7,8 6,9 10 1,4,11 5 2,3,7,8 6,9 1,4 10 5 2,3,7,8 1,4 6,9 5 1,4 6 2,3,7,8 5 1,4 6 2,3,7
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[COSSZ’19]
✓
1,3 2 4 5,6
,
5 2,3 6 1,4
◆
1 2 3 4 5 6 1 2 3 4 5 6
Generalized permutation of propagating blocks:
- !
✓{2, 3} {1, 4} {6} {5, 6} {2} {4} ◆ non-propagating blocks: {5}, {1, 3} Insertion Tableau Recording Tableau ; ; {5, 6}!
5,6 2,3
{2} !
2 5,6 2,3 1,4
{4} !
2 4 5,6 1,3 2,3 6 1,4 5
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Many Nice Properties
here are a few
- 1. Reflect the diagram over its horizontal axis:
d =
- !
(P, Q) flip(d) =
- !
(Q, P)
- 2. Consequence: |{symmetric diagrams}| = P
λ dim(Pλ k).
Implies: a “model” representation on symmetric diagrams ([H-Reeks’15]).
- 3. Respects subalgebras:
$
· · · 1 2 5 8 3 4 9 6 7
$
· · · 1, 5 6, 9 2 4 7 3 8
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